|Publication number||US4587482 A|
|Application number||US 06/519,733|
|Publication date||May 6, 1986|
|Filing date||Aug 2, 1983|
|Priority date||Aug 2, 1983|
|Publication number||06519733, 519733, US 4587482 A, US 4587482A, US-A-4587482, US4587482 A, US4587482A|
|Original Assignee||Mitsubishi Denki Kabushiki Kaisha|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (4), Non-Patent Citations (4), Referenced by (3), Classifications (11), Legal Events (4)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This invention relates to a digital frequency meter for use in radiation monitors which are installed in a nuclear power station, etc.
A prior-art apparatus of this type has been as illustrated in FIGS. 1A and 1B. In FIG. 1A, numeral 1 designates a present counter, numeral 2 a timer, and numeral 3 a computer.
Pulses to be measured are applied to the present counter 1, and are counted to a present number (denoted by N). The timer 2 measures the period of time (denoted by T) taken for the preset counter 1 to count the N pulses to-be-measured.
The quantities N and T are inputted to the computer 3, and the frequency of the pulses to-be-measured is obtained via the following calculation: ##EQU1##
FIG. 1B shows an example of the operating waveforms of the apparatus shown in FIG. 1A. The computer 3 generates a measurement start pulse PSTART at a time ts1. This pulse PSTART resets the preset counter 1 and the timer 2 into the initial statuses thereof. Thenceforth, the preset counter 1 counts the pulses to-be-measured, and the timer 2 counts reference time pulses (not shown), to increase their count values. When the count content of the preset counter 1 has reached the preset value N at time tE1, this preset counter generates a measurement end pulses PEND. This pulse PEND stops the counting operation of the timer 2, and informs the computer 3 of the end of the measurement. Upon receiving the pulse PEND, the computer 3 executes a series of operations including the loading of the count value T1 of the timer 2, the calculation of the frequency, the updating of the frequency output, and the generation of the measurement start pulse PSTART at a time ts2.
By repeating the above operations, the frequency of the pulses to-be-measured is measured.
Since the prior-art digital frequency meter is constructed and operated as described above, it requires the counter for counting the pulses to-be-measured and the timer having a dynamic range equivalent, at least, to that of the rate of the pulses to-be-measured and the division is necessary within the computer. Another disadvantage is that the frequency which is outputted every cycle of sampling changes discontinuously. Particularly in case of a low frequency, the sampling cycle becomes long, and the discontinuous change of the frequency to be outputted every sampling cycle is unfavorable for the radiation monitor for which the monitoring of the slow variation of a radiation level is also important.
This invention has been made in order to eliminate the disadvantages of the prior-art apparatus as described above, and has for its object to provide a digital frequency meter whose frequency output changes continuously and whose statistical error becomes constant.
FIG. 1A is a block diagram showing the arrangement of a prior-art digital frequency meter, while FIG. 1B is an operating waveform diagram thereof;
FIG. 2 is a block diagram showing the arrangement of a digital frequency meter according to an embodiment of this invention;
FIG. 3 is a table showing the input/output characteristics of a rate multiplier in the embodiment;
FIG. 4 is a table showing the input/output characteristics of a ROM in the embodiment;
FIG. 5 is a simplified block diagram of the digital frequency meter embodying this invention; and
FIG. 6 is a block diagram illustrative of the response characteristics of the digital frequency meter embodying this invention.
Now, an embodiment of this invention will be described with reference to the drawings.
In FIG. 2, numeral 4 designates a clock generator, which delivers a pulse train of frequency Fx as its output. Numeral 5 designates a rate multiplier, which is exemplified as consisting of 16 bits. The output pulses of frequency FB of the rate multiplier 5 is a function of its inputs M0 -M15 and the frequency Fx. That is: ##EQU2## where M: logical value "1" or "0" of the inputs M0 -M15,
The relations between the inputs M0 -M15 and the output pulses of frequency FB in the case of assuming the frequency Fx of the clock generator 4 to be 65536 are listed in FIG. 3. Numeral 6 in FIG. 2 indicates a first up/down counter, the UP input of which is supplied with pulses to-be-measured of frequency FIN and the DOWN input of which is supplied with the output pulses of frequency FB of the rate multiplier 5. The first up/down counter 6 integrates the differences between its input pulses of frequencies FIN and FB. More specifically, in case of FIN >FB, the counter 6 counts up, and it generates a carry output C each time an overflow arises. In case of FIN <FB, it counts down, and it generates a borrow output B each time an underflow arises. In case of FIN =FB, it repeats the countup and coundown alternately and generates neither the carry output C nor the borrow output B. Shown at numeral 7 is a second up/down counter, the UP input of which is supplied with the carry output C of the first up/down counter 6 and the DOWN input of which is supplied with the borrow output B. Likewise to the first up/down counter 6, the second up/down counter 7 integrates the differences between its UP signals and DOWN inputs. The instantaneous value of the integration is delivered as a binary number which is expressed by the combination of the logical values "1" or "0" of outputs Q0 -Q11.
Numeral 8 indicates a ROM (read only memory), the address inputs A0 -A11 of which are respectively supplied with the outputs Q0 -Q11 of the second up/down counter 7. Data appointed by the address inputs A0 -A11 are delivered to data outputs φ0 -φ15. In the illustrated case of FIG. 2, the ROM 8 has the address inputs of 12 bits and the data outputs of 16 bits. That is, this ROM can generate data of 16 bits in a number of 212 =4096. The output data φ0 -φ15 of the ROM 8 are applied to the inputs M0 -M15 of the rate multiplier 5, and then simultaneously used as a frequency output.
Letting A denote the input value of the address inputs A0 -A11 of the ROM 8, this ROM is programed so that the relationship between the value A and the data output φ may become as given by the following formula:
φ: data output value of the ROM 8,
A: address input value of the ROM 8,
m: value determined by selecting the maximum value φm of φ and the maximum value Am of A, that is, ##EQU3## holds from above. FIG. 4 lists some relations between the address inputs A and the data outputs φ in the case of selecting φm=65535 and Am=4095. The data outputs φ of the ROM 8 are applied to the inputs M of the rate multiplier 5 so as to control the output frequency FB. A closed loop which is constructed of the rate multiplier 5, first up/down counter 6, second up/down counter 7 and ROM 8 acts so as to equalize the frequencies FIN and FB. The output φ of the ROM 8 at the time at which the frequencies FIN and FB have equalized is a function of FB and FIN, and is therefore used as the frequency output.
FIG. 5 shows the closed loop as an equivalent block diagram. A block 51 represents the combined function of the first up/down counter 6 and second up/down counter 7, and indicates integrating the differences between FIN and FB. A block 52 represents the combined function of the ROM 8 and rate multiplier 5.
In the block 52, letter r indicates the count capacity of the first up/down counter 6. Each time the integrated value of the differences between the UP inputs (FIN) and DOWN inputs (FB) becomes r, the carry output C or borrow output B is generated. Letter c indicates the instantaneous value of the integrated value of the second up/down counter 7.
FIG. 6 shows a block diagram of a transfer function in which the block diagram of FIG. 5 is expressed by the Laplace function. A block 51a expresses the block 51 as the Laplace function, and a block 52a the block 52. Letter K indicates the instantaneous value of mc/r.
In FIG. 6, the transfer characteristic from the frequency FIN to the frequency output is given by the following formula: ##EQU4## The frequency output of the steplike change of FIN is given by the following formula: ##EQU5## When this is subjected to the inverse Laplace transform, the frequency output expressed as a time function is given by the following formula:
Frequency output (t)=F.sub.IN (1=e.sup.-kt)
Thus, it is understood that the frequency output responds to the step change of the input FIN with a time constant=1/K, which is the inverse value of the gain K of the block 52a. In addition, the gain K is expressed by the ratio of the change of FB to the change of FIN, that is, ##EQU6## Since the gain K expresses the instantaneous value of mc/r as stated before, it changes depending upon the value of c. Accordingly, the time constant changes depending upon the value of c.
Now, the variation ΔFB of FB with respect to the variation ΔFIN =1 of FIN will be evaluated. Since the input FIN has been diminished to 1/r by the first up/down counter 6, the variation ΔFB is given by the following formula: ##EQU7## Since the instantaneous value of the gain is ΔFIN =1, it is expressed by the following formula: ##EQU8## Accordingly, the time constant τ at this time is expressed by the following formula: ##EQU9##
On the other hand, since FB =(m)c/r
is set, τ is also expressed as follows: ##EQU10## It is also understood that the time constant τ is inversely proportional to FB because ##EQU11## is a constant. That is, at the equilibrium point of the closed loop, the time constant of this closed loop is inversely proportional to the frequency of the pulses to-be-measured.
Meanwhile, it is known that a statistical deviation σ at the measurement of radiation with a frequency meter is given by the following formula: ##EQU12## where τ: time constant of the frequency meter,
n: frequency of the pulses to be measured.
Since FB is proportional to the frequency n of the pulses to-be-measured, ##EQU13## holds, and this becomes a constant value irrespective of the frequency. It is accordingly understood that the frequency output whose statistical deviation is constant irrespective of the frequency is obtained. By setting r variably, the statistical deviation can be varied.
As set forth above, according to this invention, the time constant of a frequency meter is inversely proportional to the frequency. This brings forth the effect that a digital frequency meter whose statistical deviation is constant irrespective of the frequency and whose frequency output changes continuously is provided.
|Cited Patent||Filing date||Publication date||Applicant||Title|
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|Citing Patent||Filing date||Publication date||Applicant||Title|
|US6470295 *||Jun 5, 1998||Oct 22, 2002||George Dieter Mirow||Method for displaying statistically occurring events|
|CN104115403A *||Oct 24, 2012||Oct 22, 2014||Abb技术有限公司||Pulse frequency measurement device and method and control system|
|CN104115403B *||Oct 24, 2012||Oct 19, 2016||Abb技术有限公司||脉冲频率测量设备和方法以及控制系统|
|U.S. Classification||324/76.64, 324/76.48, 327/48, 324/76.17, 324/77.11|
|International Classification||G01R19/252, G01R23/02|
|Cooperative Classification||G01R19/252, G01R23/02|
|European Classification||G01R19/252, G01R23/02|
|Sep 6, 1983||AS||Assignment|
Owner name: MITSUBISHI DENKI KABUSHIKI KAISHA 2-3, MARUNOUCHI
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST.;ASSIGNOR:HASEGAWA, MASAKOTO;REEL/FRAME:004165/0854
Effective date: 19830715
|Oct 30, 1989||FPAY||Fee payment|
Year of fee payment: 4
|Oct 25, 1993||FPAY||Fee payment|
Year of fee payment: 8
|Sep 29, 1997||FPAY||Fee payment|
Year of fee payment: 12